During distance running, a runner must perceive the salient features of the environment and modulate the movement pattern in order to successfully displace the body. A runner selects a movement pattern based upon many different factors. For example, surface characteristics, running shoes, body structure, physiological state and desired running velocity are factors that could influence a runner’s movement pattern. Ultimately, the movement pattern selected determines how economical a runner is from a physiological perspective - and running economy is an important aspect of distance running performance (Hogberg, 1952; Cavanagh and Williams, 1982; Cavanagh and Kram, 1985; Hamill et al. 1995).

During running, the ground reaction force, gravity and air resistance are the forces acting on the runner. While gravity is a constant force and air resistance force is of small magnitude, the ground reaction force is of high magnitude and varies based upon a variety of factors such as running velocity and running style. Therefore, it is understandable that there is a wealth of research on factors that influence ground reaction forces during running since this parameter ultimately provides some insight into running behavior.

The ground reaction force is typically analyzed by decomposing the resultant force vector into two shear components (i.e., anterior-posterior, medial-lateral) and a vertical component. The focus of this paper is on the vertical ground reaction force since it is the dominant force in terms of magnitude. There are many interesting characteristics of a vertical ground reaction force profile during running, but an important aspect of the force profile that is the impact force (i.e., F1, Figure 1a), which is the local maximum force generally observed within about 50 ms of ground contact (Nigg et al., 1995). A reason for the interest in the impact force is due to the hypothesis that running overuse injuries are related to the collision between the foot and ground with each foot-strike (Hreljac et al., 2000).

Impact force magnitudes are influenced by running velocity such that force magnitudes increase with faster velocities (Hamill et al., 1983; Munro et al., 1987; Mercer and Vance, 2002). Impact force magnitudes are also influenced by changes in stride length (Derrick et al., 2000; Challis, 2001) such that force magnitudes increase with longer stride lengths. During running, this impact force is absorbed through joint actions as well as anatomical structures. The process of reducing the impact force is referred to as impact attenuation (Hamill et al., 1995; Derrick et al., 1998; Mercer et al., 2002a). Similar to impact force, impact attenuation increases with faster running velocities (Mercer et al. 2002b) and longer stride lengths for a given velocity (Hamill et al., 1995; Derrick et al., 1998).

In general, faster submaximal running velocities are accomplished primarily by changes stride length (Sinning and Forsyth, 1970; Luhtanen and Komi, 1978; Mercer et al., 2002b), which leads to the question: Are the changes in impact characteristics (i.e., impact force magnitude and impact attenuation) across velocities related to stride length changes?

Lower extremity geometry at impact has been related to impact force magnitude (Denoth, 1983; Gerritsen et al., 1995; Lafortune et al., 1996) as well as impact attenuation (Derrick et al., 1998; 2000). It seems reasonable to suspect that stride length imposes a constraint to lower extremity geometry at impact. Although there is a wealth of documentation regarding ground reaction forces during running, there is very little research on the effect of stride length changes on these forces. Therefore, the purpose of this study was to investigate whether or not stride length influences the relationship between running velocity and impact characteristics (i.e., impact magnitude and impact attenuation). The experiment that we designed to address this purpose consisted of having participants run at a variety of velocities with stride length either freely chosen or constrained by striking specific targets. The hypothesis that impact force is related to changes in stride length (regardless of velocity) would be rejected if impact force changed in a similar manner during both stride length conditions.

Volunteers (n = 8, mean standard deviation: mass = 72.4 ± 8.9 kg; height = 1.7 ± 0.1 m; age = 25 ± 3.4 years) gave written informed consent to participate in the study. All participants completed all running conditions and did not have any injury that interfered with running performance.

Subjects were provided a laboratory running shoe (Asics American Corporation, Irvine, CA; model TN 415) to wear during testing. Ground reaction forces were measured using a force plate (Kistler Instrument Corporation USA, Amherst, NY; model 9281B) that was mounted flush with the floor in the middle of a 20 m runway. Impact attenuation was quantified by securing light weight uni-axial accelerometers (PCB Piezotronics, Depew, NY; model 353C67; mass = 2 grams; sensitivity = 100 mV·g-1; frequency range = 0.3 Hz - 12 kHz) on the right leg and head segments. The leg accelerometer was mounted on the distal anterior-medial aspect of the tibia using a custom wrap tightened to subject tolerance level. The head accelerometer was fixed to a rigid plastic head gear that was similar to a hat band and could be tightened around the head such that the accelerometer was aligned vertically in the middle of the forehead region. Running velocity was determined using two infrared photo sensors (Lafayette Instrument Corporation. USA, Lafayette, IN; model 63501IR) that triggered a signal when the participant ran past a sensor. Sensors were placed 1.5 m before and after the force plate in order to determine running velocity. All data were collected concurrently at 1080 Hz using Bioware (Kistler Instrument Corporation, Depew, NY; version: 3.21) data acquisition software.

The goal of this experiment was to record ground reaction force and acceleration data during running at a variety of velocities when stride length was either self-selected or constrained. Therefore, participants completed multiple trials during each of two conditions: 1) preferred stride length (PSL), 2) stride length constrained to 2.5 m (SL2.5). Condition order was always PSL - SL2.5 since it was felt that constraining stride length may interfere with the natural self-selection of stride length. During PSL trials, no instructions regarding stride length were provided, while during SL2.5 participants were required to strike floor targets such that stride length would always be 2.5 m. The stride length of 2.5 m was chosen knowing that during slow speeds this stride length would be longer than a subject would normally choose and, likewise, would be shorter than a subject would normally choose while running faster speeds. Nevertheless, we chose this stride length based upon pilot work and we believed would allow subjects to achieve a wide range of running speeds.

During each condition, the goal was to collect 20 trials representing a variety of speeds such that the distribution of speeds was similar between conditions. For each condition, participants were instructed to run at a comfortable pace at first. A member of the research team then gave instructions to the participant to either increase or decrease velocity with the intent of recording a wide range of velocities that would be similar between conditions. During PSL, a successful trial required that the participant struck the force plate with the right foot and did not make any obvious changes to stride length in order to strike the force plate. During SL2.5, a successful trial required that the participant struck the force plate with the right foot and struck targets placed on the ground at specific intervals. A participant was allowed no more than 40 attempts per condition to achieve 20 successful trials. Data sets for two subjects were dropped from the study since the velocity distributions were not similar between conditions. This resulted in an analysis of data sets from 6 subjects (mass = 74 ± 9.5 kg; height = 1.7 ± 0.1 m; age = 26 ± 4.0 years). Of these six subjects, five completed 20 trials per condition while one completed 15 trials per condition.

The targets for SL2.5 were placed such that stride length would be 2.5 m. Markers were placed on the floor at 1.25 m intervals so that the participant could target left and right foot strikes. During the SL2.5 trials, different running velocities were achieved by manipulating stride frequency.

A typical trial data set consisting of force and acceleration data is illustrated in Figures 1a, 1b, and 1c. Running velocity was calculated by processing the square wave signals generated by each timing sensor triggered by the participant running through the test area. Leg and head acceleration data were smoothed using a 4^th order, zero-lag Butterworth filter (cutoff frequency = 50 Hz). Stride length was determined by first identifying two consecutive leg peak impact accelerations (Figure 1c). The time between peaks was used to calculate stride frequency (strides·s^-1) with stride length then calculated by dividing running velocity by stride frequency.

The impact force (F1, Figure 1a) from the vertical ground reaction force profile was recorded as well as the average vertical force during the stance phase. A force threshold of 20 N was used to identify contact and toe-off times of the force profile. We also calculated the resultant impact force (Fr) and direction (θ¸) of this force using the vertical and anterior-posterior forces. Finally, the head peak impact acceleration (a_head; Figure 1b) as well as the leg peak impact acceleration (a_leg; Figure 1c) associated with contact of the force plate were recorded (Figure 1) and used to calculate impact attenuation using the formula: impact attenuation = (1- a_head/ a_leg) 100.

Scatter plots of each parameter vs. running velocity were generated for each condition for each participant. A line of best fit was calculated for each parameter per condition per participant with the slope of this line recorded for analysis. For example, the impact force for each trial of PSL for participant 1 was plotted against running velocity. A line of best fit (i.e., y = mx + b; where m = slope and b = the y intercept) was calculated and the slope of this line was recorded for analysis. This procedure was repeated for all participants and all conditions for each parameter of interest.

The primary dependent variables were the slopes of impact force vs. running velocity (m_F1) and impact attenuation (m_IA) vs. running velocity relationships. Stride length condition (i.e., PSL, SL2.5) was the independent variable. In addition to these dependent variables, the slopes for average vertical force (m_Favg), resultant impact force (m_Fr), direction of resultant force (m_θ¸), stance time (m_st), a_leg (m_leg), and ahead (m_head) were also compared between stride length conditions (i.e., PSL, SL2.5). Paired t-tests were used to compare each dependent variable between the two stride length conditions (α= 0.05).

The velocities were distributed in a similar manner between conditions (PSL: 3.6 ± 0.1 m·s^-1; SL2.5: 3.5 ± 0.1 m·s^-1; p > 0.05). Stride length increased with running velocity during PSL but not during SL2.5 (Figure 2, Table 1, p < 0.05), indicating that we achieved our goal of similar running velocity distributions between conditions as well as achieving our stride length manipulation goal.

The slope for each force parameter (m_F1, m_Favg, m_Fr) vs. running velocity relationship was different between conditions, with the slopes being greater during PSL vs. SL2.5 for each parameter (Table 1, p < 0.05). The slope of resultant force direction (m_θ¸) was not different between stride length conditions (Table 1, p > 0.05). Figure 3 illustrates the relationship between vertical impact force and running velocity for each condition.

The slope of the impact attenuation (m_IA) vs. running velocity relationship was greater during PSL compared to the slope during SL2.5 (Figure 4, p < 0.05). Neither of the slopes for a_leg (m_leg) or a_head (m_head) were different between stride length conditions (Table 1, p < 0.05).

Previous studies have determined that ground reaction forces change as running velocity changes (Hamill et al., 1983; Munro et al., 1987; Mercer and Vance, 2002). The basic kinematic descriptors of running behavior are stride length and stride frequency. In general, faster submaximal running velocities are achieved primarily by increases in stride length (Sinning and Forsyth, 1970; Luhtanen and Komi, 1978; Mercer et al., 2002b). Since stride length changes concurrently with changes in running velocity and changes in stride length influence impact force for a given running velocity (Derrick et al., 2000; Challis, 2001), it was not clear whether impact force changes due to velocity or stride length changes. By manipulating running velocity and either allowing stride length to naturally change or constraining stride length, we observed that stride length is critically related to impact force magnitude.

We observed that the impact force increased 0.178 BW/m·s^-1 when stride length was freely chosen (i.e., PSL) across velocities ranging from about 2.5 m·s^-1 to about 5.5 m·s^-1. This relationship is similar to the impact force vs. running velocity relationship observed by Mercer and Vance (2002; 0.23 BW/m·s^-1) but lower than other studies (0.41 BW/m·s^-1; Hamill et al., 1983; 0.38 BW/m·s^-1 Munro et al., 1987). Nevertheless, when stride length was constrained, the slope of the impact force-velocity relationship was dramatically different (-0.003 ± 0.14 BW/m·s^-1) than during PSL (0.178 ± 0.16 BW m·s^-1).

We considered that our study was limited by the analysis of data sets from six subjects. For example, one subject had no increase in impact force during PSL while impact force increased while stride length was constrained for a different subject. Previously, our laboratory had conducted a similar study (Mercer et al., 2001) where stride length was allowed to vary or was constrained at 2.5 m and 3.0 m. In that study (n = 10), it was also observed that the relationship between impact force and running velocity was influenced by constraints on stride length. Furthermore, combining the results from the current study with the 2.5 m data from the previous study yielded the same statistical outcome. However, we ultimately did not combine the two data sets for this study since acceleration data were not collected for those ten subjects.

In our study, impact attenuation increased with faster running velocities when stride length was allowed to vary. This was expected since it is well established that impact attenuation increases with faster running velocities (Shorten and Winslow, 1992; Mercer et al., 2002b). Mathematically, impact attenuation changed across velocities due to an increase in leg impact acceleration not head impact accelerations (Table 1). The leg impact accelerations tended to increase (p = 0.10) about 24% per m·s^-1, which is lower than the 42% and 34% increase in leg impact acceleration per m·s^-1 reported by Mercer et al. (2002b) and Clark et al. (1985), respectively. When stride length was constrained, there was no direct relationship between leg impact acceleration and running velocity. In contrast, the head impact acceleration relationship did not differ between stride length conditions. This was expected since head impact accelerations typically do not vary drastically between a variety of running conditions (e.g., Derrick et al., 1998; Derrick et al., 2002; Mercer et al., 2002a; Mercer et al., 2002b; Mercer et al., 2003) - which supports the hypothesis that anatomical structures and kinematic strategies result in attenuating impact frequencies (Hamill et al., 1995).

The importance of stride length changes on impact force and impact attenuation is that stride length is likely related to the lower extremity posture at impact. Simulated impact magnitudes have been related to lower extremity geometry at impact (Denoth, 1983; Gerritsen et al., 1995) and impact attenuation has been related to the distance between the direction of the line of action of the resultant ground reaction force and knee joint center (Derrick et al., 1998; 2004). Given that the slope of the direction of Fr (i.e., m_θ¸) was not influenced by stride length condition, it is conjectured that impact characteristics (i.e., impact force magnitude and impact attenuation) were influenced by the lower extremity posture at impact. Specifically, it is conjectured that the lower extremity posture remained the same when stride length was constrained but changed when stride length was allowed to be freely chosen (i.e., PSL). Future research combining kinetic and kinematic information is needed to address this hypothesis.

Running is a complex movement pattern that is accomplished with very little conscious thought. As running velocity is increased it is expected that running behavior changes. We observed that stride length increased with faster running velocities during the PSL condition, which is similar to other studies (Sinning and Forsyth, 1970; Luhtanen and Komi, 1978; Mercer et al., 2002b). This leads to an interesting question: Why do runners choose to increase stride length to achieve faster submaximal running velocities? From our study, it does not seem that running behavior is based upon regulating impact force or impact attenuation since both parameters increased with faster running velocities when stride length was self-selected (i.e., PSL). Furthermore, as illustrated in Figure 3 (impact force vs. velocity), runners could select a stride length that results in a lower impact force than the freely chosen stride length. Hamill et al. (1995) also concluded that running behavior for a single velocity was not a function of impact attenuation. It may be, instead, that there is a target stride frequency that is being maintained across velocities.

We observed that stride frequency changed very little across a variety of submaximal running velocities during the PSL condition, which is a similar observation to other studies (Sinning and Forsyth, 1970; Luhtanen and Komi, 1978; Mercer et al., 2002b). It has been hypothesized that there is an optimal stride frequency that results in a minimal amount of oxygen consumption when running a given velocity (Hogberg, 1952; Cavanagh and Williams, 1982; Hamill et al., 1995). It may be that running behavior across velocities is based upon maintaining an optimal stride frequency, and changes to stride length are therefore a consequence to maintaining stride frequency. The importance of maintaining stride frequency may be related to the importance of selecting a movement pattern best suited for coordination of lower extremity movements that result in an economical movement pattern. In any case, a consequence of maintaining stride frequency across different velocities is increased impact force only because stride length is changing. Interestingly, despite increases in impact force, the runner seems to always absorb sufficient impact energy such that head impact accelerations are nearly constant despite a variety of impact force magnitudes. It may be that maintaining a stable visual field is a criteria driving running behavior.

There is a wealth of published research investigating factors that influence the ground reaction forces during running since these forces are likely related to overuse injuries commonly observed in runners and these are the forces that cause movement. We conducted an experiment in which ground reaction forces were analyzed across different velocities when subjects were allowed to either self-select stride length (PSL) or run with a specific stride length (i.e., SL2.5 m). We observed that stride length was an important factor that determined impact force magnitude. Future research is needed to determine which aspects of stride length are important determinants of impact characteristics.